Transmission method, transmission apparatus, reception method and reception apparatus
a transmission apparatus and reception method technology, applied in the field of transmission apparatus, transmission apparatus, reception method and reception apparatus, can solve the problems of high field strength, degradation of reception quality, and achieve the effect of improving reception quality and deterioration of reception quality in los environments
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embodiment 1
[0134]The following describes the transmission method, transmission device, reception method, and reception device of the present embodiment.
[0135]Prior to describing the present embodiment, an overview is provided of a transmission method and decoding method in a conventional spatial multiplexing MIMO system.
[0136]FIG. 1 shows the structure of an Nt×Nr spatial multiplexing MIMO system. An information vector z is encoded and interleaved. As output of the interleaving, an encoded bit vector u=(u1, . . . , uNt) is acquired. Note that ui=(ui1, . . . , uiM) (where M is the number of transmission bits per symbol). Letting the transmission vector s=(s1, . . . , sNt)T and the transmission signal from transmit antenna #1 be represented as si=map(ui), the normalized transmission energy is represented as E{|si|2}=Es / Nt (Es being the total energy per channel). Furthermore, letting the received vector be y=(y1, . . . , yNr)T, the received vector is represented as in Equation 1.
Math1y=(y1,…,yNr)...
embodiment 2
[0277]In Embodiment 1, regular hopping of the precoding weights as shown in FIG. 6 has been described. In the present embodiment, a method for designing specific precoding weights that differ from the precoding weights in FIG. 6 is described.
[0278]In FIG. 6, the method for hopping between the precoding weights in Equations 37-40 has been described. By generalizing this method, the precoding weights may be changed as follows. (The hopping period (cycle) for the precoding weights has four slots, and Equations are listed similarly to Equations 37-40.) For symbol number 4i (where i is an integer greater than or equal to zero):
Math42(z1(4i)z2(4i))=12(jθ11(4i)j(θ11(4i)+λ)jθ21(4i)j(θ21(4i)+λ+δ))(s1(4i)s2(4i))Equation42
Here, j is an imaginary unit.
For symbol number 4i+1:
Math43(z1(4i+1)z2(4i+1))=12(jθ11(4i+1)j(θ11(4i+1)+λ)jθ21(4i+1)j(θ21(4i+1)+λ+δ))(s1(4i+1)s2(4i+1))Equation43
For symbol number 4i+2:
Math44(z1(4i+2)z2(4i+2))=12(jθ11(4i+2)j(θ11(4i+2)+λ)jθ21(4i+2)j(θ21(4i+2)+λ+δ))(s1(4i+2)s2(4i+...
example # 1
Example #1
[0290](1) θ11(4i)=θ11(4i+1)=θ11(4i+2)=θ11(4i+3)=0 radians,
(2) θ21(4i)=0 radians,
(3) θ21(4i+1)=π / 2 radians,
(4) θ21(4i+2)=π radians, and
(5) θ21(4i+3)=3π / 2 radians.
(The above is an example. It suffices for one each of zero radians, π / 2 radians, π radians, and 3π / 2 radians to exist for the set (θ21(4i), θ21(4i+1), θ21(4i+2), θ21(4i+3)).) In this case, in particular under condition (1), there is no need to perform signal processing (rotation processing) on the baseband signal S1(t), which therefore offers the advantage of a reduction in circuit size. Another example is to set values as follows.
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